H. Shao, Y.-B. Tang, H.-L. Yue, F.-F. Wu, Z.-X. Ma, Y. Huang, L.-Y. Tang, H. Guan, K.-L. Gao, "Precision determination of dipole transition elements with a single ion," Photonics Res. 12, 2242 (2024)

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- Photonics Research
- Vol. 12, Issue 10, 2242 (2024)

Fig. 1. (a) Sketch of the experimental setup for dipole transition matrix elements with single trapped ion. (b) Yb + energy-level diagram of low-lying states (not to scale), where r denotes the branching fraction of the 6 p P 1 / 2 2 state into the 5 d D 3 / 2 2 state.

Fig. 2. Simplified time sequence and associated energy level diagram (not to scale) displaying the 6 p P 1 / 2 2 -5 d D 3 / 2 2 spontaneous decay rate measurements in a single Yb + ion.

Fig. 3. The data points are fitted to determine key decay parameters. (a) The fitting curve for the decay parameter b at each 369 nm power p through decay probability P and its pulses duration time by using an exponential function Eq. (2 ). (b) The fitting curve for the spontaneous decay rate A P D through variational decay parameter b and its corresponding laser power p by using Eq. (4 ). (c) The spontaneous decay rate A P D is exponentially plotted against the detuning of the 369 nm laser frequency from the resonance frequency of the 6 p P 1 / 2 2 -6 s S 1 / 2 2 transition. The shown data in (a) and (b) correspond to the point in (c) where the detuning is −6 MHz. The transition probability at the resonance frequency is determined to be 0.62796(81) μs − 1 .

Fig. 4. Comparison of experimental and theoretical branching fractions for the 6 p P 1 / 2 2 -5 d D 3 / 2 2 transition in Yb + .

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